Image reconstruction by OPED algorithm with averaging

OPED is a new image reconstruction algorithm based on orthogonal polynomial expansion on the disk. We show that the integral of the approximation function in OPED can be given explicitly and evaluated efficiently. As a consequence, the reconstructed image over a pixel can be effectively represented by its average over the pixel, instead of by its value at a single point in the pixel, which can help to reduce the aliasing caused by under sampling. Numerical examples are presented to show that the averaging process indeed improves the quality of the reconstructed images. The work of the first author is supported in part by the National Science Foundation under Grant DMS-0604056.     

基于细菌视紫红质薄膜的空间光调制器实验研究

阐述了利用细菌视紫红质薄膜（BR薄膜）优良的非线性光学特性作为光寻址的空间光调制器的实验研究.BR有两个重要的光敏中间态（B态和M态），其吸收带（B态吸收峰为570nm，M态吸收峰为412nm）重叠区域较少，利用其正向（B→M）和逆向（M→B）光反应之间转化关系和B态与M态的差异吸收实现了相干光学图像到非相干光学图像的转换实验.采用经基因改性的细菌视紫红质薄膜（BRD96N）材料，使用670nm相干光作为写入光，530nm非相干光作为读出光，得到了分辨率约为200 lines/mm，对比度约为2.1∶1的 关键词： 光寻址空间光调制器 细菌视紫红质薄膜（BR薄膜） 非线性光学特性 相干光与非相干光图像相互转换     

行列式为零的光学元件及其可能应麟

一种行列式为零的新元件具有广角、无穷是深和均匀照明的特点.应用前景是诱人的.     

对固定平台红外单站被动定位技术研究

介绍了一种基于红外成像和序列图像处理技术的对固定平台红外单站被动定位新算法.该算法通过对红外成像目标的实时测量信息求解出目标相对测量基站的距离,它适用于匀速、匀加速和变加速等各种运动模型,具有定位精度高、体积小和便于机动的特点.该算法对可见光成像单站被动定位同样有效.     

实用型模块化成像光谱仪多光谱图像的信噪比估算及压缩方法研究

采用局部标准差法和去相关法对实用型模块化成像光谱仪多光谱图像的信噪比进行估算。这两种方法已将地物变化的影响降低到很低的程度。这样在大气订正后，图像的信噪比性能充分反映出遥感仪器的信噪比性能。针对图像压缩，提出控制各波段恢复图像的峰值信噪比刚好大于原始图像的信噪比，使由压缩算法本身所带来的噪声限制在原始图像的噪声范围之内。结合这种压缩思想，用基于离散余弦变换和基于离散小波变换的压缩算法，对实用型模块化成像光谱仪多光谱图像进行压缩。实验表明，利用这种方法，对于高信噪比的波段，图像信息得到了保真；对低信噪比的波段，压缩倍数提高迅速且恢复图像视觉无失真，对整幅成像光谱图像，压缩性能提升显著——当压缩比等于37．95倍时，峰值信噪比等于45．86dB。     

Theoretical study of laser light generation and color image formation: FA1:Cs+ and FA2:Li+ centers at the low coordination (100) and (110) surfaces of AgCl and AgBr

The F_A1:Cs⁺ and F_A2:Li⁺ color centers at the low coordination (100) and (110) surfaces of AgCl and AgBr play important roles in laser light generation and color image formation. Double‐well potentials at these surfaces are investigated by using ab initio calculations. Quantum clusters were embedded in the simulated Coulomb fields that closely approximate the Madelung fields of the host surfaces, and ions that are the nearest neighbors to the F_A ? defect site are allowed to relax to equilibrium. The calculated Stokes shifts suggest that laser light generation is sensitive to the simultaneous effects of the vibrational coupling mode, the impurity cation, the coordination number of the surface ion, the lattice anion, and the choice of the basis set centered on the anion vacancy. An attempt has been made to explain these effects in terms of Madelung potential, electron affinity, and optical–optical conversion efficiency. All relaxed excited states of the defect‐containing surfaces are deep below the lower edges of the conduction bands of the ground‐state defect‐free surfaces, suggesting that the F_A(I):Cs⁺ and F_A(II):Li⁺ centers are suitable laser defects. The dependence of orientational destruction, recording sensitivity, and exciton (energy) transfer on the empty cation; the coordination number of the surface ion; and the lattice anion is clarified. The Glasner–Tompkins empirical rule was generalized to include the impurity cation and the coordination number of the surface ion. As far as color image formation is concerned, the supersensitizer was found to increase the sensitizing capabilities of two primary dyes in the excited states by increasing the relative yield of quantum efficiency. The (110) surfaces of AgBr and AgCl were more sensitive than the corresponding (100) surfaces, and AgBr thin film was found to be more sensitive than that of AgCl. On the basis of quasi‐Fermi levels, the difference in the sensitizing capabilities between the examined dyes in the excited states is determined. © 2005 Wiley Periodicals, Inc. Int J Quantum Chem, 2005